ar X iv : n uc l - th / 9 81 10 52 v 3 1 8 N ov 1 99 8 Carbon Isotopes Near Drip Lines in the Relativistic Mean - Field Theory

ar X iv : n uc l - th / 9 81 10 23 v 1 8 N ov 1 99 8 Mean – Field and Nonlinear Dynamics in Many – Body Quantum Systems

In this paper we discuss in detail the nonlinear equations of the mean–field approximation and their connection to the exact many–body Schrödinger equation. Then we analyze the mean–field approach and the nonlinear dynamics of a trapped condensate of weakly–interacting bosons.

v 1 1 5 N ov 1 99 8 Carbon Isotopes Near Drip Lines in the Relativistic Mean - Field Theory

We have investigated the ground-state properties of carbon isotopes in the framework of the relativistic mean-field (RMF) theory. RMF calculations have been performed with the non-linear scalar self-coupling of the σ meson using an axially symmetric deformed configuration. We have also introduced the vector self-coupling of the ω meson for the deformed mean-field calculations. The results show ...

ar X iv : n uc l - th / 9 60 80 57 v 2 1 8 N ov 1 99 6 Strong decays of nonstrange q 3 baryons

ar X iv : n uc l - th / 9 81 10 45 v 1 1 2 N ov 1 99 8 Alternative evaluations of halos in nuclei

Data for the scattering of 6 He, 8 He, 9 Li, and 11 Li from hydrogen are analyzed within a fully microscopic folding model of proton-nucleus scattering. Current data suggest that of these only 11 Li has a noticeable halo. The available data for the 6 Li(γ, π +) 6 He gs reaction support the conclusion that 6 He does not.

N ov 1 99 8 Carbon Isotopes Near Drip Lines in the Relativistic Mean - Field Theory

We have investigated the ground-state properties of carbon isotopes in the framework of the relativistic mean-field (RMF) theory. RMF calculations have been performed with the non-linear scalar self-coupling of the σ meson using an axially symmetric deformed configuration. We have also introduced the vector self-coupling of the ω meson for the deformed mean-field calculations. The results show ...